Interpreting the coefficients of the endogenous variables in IV models

Author

Giovanni Forchini

Published

July 18, 2017

In the simple linear model \(y=x \beta +u\), the (scalar) parameter \(\beta\) has a very simple interpretation:

\[\frac{\partial E\left( y|x \right)}{\partial x} = \beta. \ \ \ \ (1)\]

That is, a marginal change in the independent variable \(x\) leads to a change \(\beta\) in \(E\left( y|x \right)\). It is natural to carry forward this interpretation to a simple linear instrumental variable models of the form

\[y=x\beta+u\] \[x=z'\gamma+v,\]

and claim that \(\frac{\partial E\left( y|x,z \right)}{\partial x} = \beta\). However, this is not the case: since \(u\) and \(v\) are dependent, a change in \(x\) may also lead to a change in \(E\left(u|x,z \right)\), which can no longer expected to be zero.

For simplicity, assume that \(\left( u , v\right)|z\) are a pair of normal random variables with zero mean and covariance matrix

\[\Sigma = \left( \begin{array}{cc} \sigma_u^2 & \rho \sigma_u \sigma_v \\\rho \sigma_u \sigma_v &\sigma_v^2 \end{array}\right).\]

Although this assumption is not needed, it helps to simplify the calculations. Focus on the pair \(\left( u,x\right)\). Notice that they are normally distributed given \(z\),

\[\left. \left(\begin{array}{c} u \\x \end{array} \right) \right| z \sim N\left(\left( \begin{array}{c} 0 \\z'\gamma \end{array}\right) , \Sigma \right).\]

So that we can easily find the conditional distribution of \(u\) given \(x\) and \(z\) as

\[u | x ,z\sim N\left( \rho \frac{ \sigma_u}{\sigma_v} \left( x-z'\gamma\right) ,\left(1-\rho^2 \right) \sigma_u^2 \right).\]

Notice that the conditional mean of \(u\) depends on \(x\) as well and on \(z\) and

\[\frac{\partial E\left( u|x,z\right) }{\partial x} =\rho \frac{ \sigma_u}{\sigma_v}.\ \ \ \ (2)\]

Now focus on the distribution of \(y\) given \(x\):

\[y|x,z \sim x\beta+u|x,z \sim N\left(x\beta+\rho \frac{ \sigma_u}{\sigma_v} \left( x-z'\gamma\right) ,\left(1-\rho^2 \right) \sigma_u^2 \right). \ \ \ \ (3)\]

Therefore

\[\frac{\partial E\left( y|x,z \right)}{\partial x} = \beta+ \rho \frac{ \sigma_u}{\sigma_v}. \ \ \ \ (4)\]

Using (2) and (4), \(\beta\) can be written as

\[\beta = \frac{\partial E\left( y|x,z \right)}{\partial x} - \frac{\partial E\left( u|x,z \right)}{\partial x}. \ \ \ \ (5)\]

Hence, \(\beta\) is the change in \(E\left( y|x,z \right)\) due to a change in \(x\) after removing the effect that \(x\) has on \(u\). A graph may be useful to understand the effect of \(x\) on \(E\left( y|x,z \right)\):

\[\begin{array}{lcccl} x & &\to & &v\\ &&&&\\ \downarrow \beta &&&&\downarrow \rho \frac{\sigma_u}{\sigma_v}\\ &&&&\\ y& &\leftarrow& &u \end{array}\]

which shows how \(x\) affects \(y\) directly (and this direct effect is \(\beta\)) and indirectly through the unobserved errors (and this effect is \(\rho \frac{\sigma_u}{\sigma_v}\)).

Pearl’s causal interpretation of \(\beta\) is slightly different since it is based on the assumption that it is possible to change \(x\) by setting it equal to a particular value and removing the reduced form \(x=z'\gamma+v\) from the system.

Notice that the assumption of normality is not needed. We could have also taken the conditional expectation on both sides of the structural equation to find

\[E\left( y|x,z\right) = x\beta+E\left( u|x,z \right).\ \ \ \ (6)\]

One obtains the earlier result by deriving with respect to \(x\) both the left and the right hand sides of (6).

I conclude this note with a few observations with which econometricians usually are not familiar: